Mass-asymmetric fission in the ⁴⁰Ca+¹⁴²Nd reaction

dc.contributor.authorEdayillam, Prasad
dc.contributor.authorHinde, David
dc.contributor.authorWilliams, Elizabeth
dc.contributor.authorDasgupta, Mahananda
dc.contributor.authorCarter, Ian
dc.contributor.authorCook, Kaitlin
dc.contributor.authorJeung, Dongyun
dc.contributor.authorLuong, Duc Huy
dc.contributor.authorMcNeil, Steven
dc.contributor.authorPalshetkar, Chandani
dc.contributor.authorRafferty, Dominic
dc.contributor.authorSimenel, Cedric
dc.contributor.authorWakhle, Aditya
dc.contributor.authorRamachandran, K.
dc.contributor.authorKhuyagbaatar, J.
dc.contributor.authorDullmann, Ch.E.
dc.contributor.authorLommel, B.
dc.contributor.authorKindler, B.
dc.contributor.editorMitchell, A.
dc.contributor.editorReed, M.
dc.contributor.editorSimpson, E.
dc.coverage.spatialCanberra
dc.date.accessioned2018-11-05T01:00:54Z
dc.date.available2018-11-05T01:00:54Z
dc.date.createdSeptember 14-18 2015
dc.date.issued2016
dc.date.updated2021-11-28T07:27:33Z
dc.description.abstractShell effects play a major role in fission. Mass-asymmetric fission observed in the spontaneous and low energy fission of actinide nuclei was explained by incorporating the fragment shell properties in liquid drop model. Asymmetric fission has also been observed in the low energy fission of neutron-deficient 180Hg nuclei in recent β-delayed fission experiments. This low-energy β-delayed fission has been explained in terms of strong shell effects in pre-scission configurations associated with the system after capture. Calculations predicted asymmetric fission for heavier Hg isotopes as well, at compound nuclear excitation energy as high as 40 MeV. To explore the evolution of fission fragment mass distribution as a function of neutron and proton numbers and also with excitation energy, fission fragment mass distributions have been measured for the 40Ca+142Nd reaction forming the compound nucleus 182Hg at energies around the capture barrier, using the Heavy Ion Accelerator Facility and CUBE spectrometer at the Australian National University. Mass-asymmetric fission is observed in this reaction at an excitation energy of 33.6 MeV. The results are consistent with the β-delayed fission measurements and indicate the presence of shell effects even at higher exciation energies
dc.description.sponsorshipThe authors acknowledge support from the Australian Research Council through grants FL110100098, FT120100760, DP130101569, DP140101337, DP160101254 and DE140100784. Support for accelerator operations through the NCRIS program is acknowledgeden_AU
dc.format.mimetypeapplication/pdfen_AU
dc.identifier.urihttp://hdl.handle.net/1885/148840
dc.publisherEPJ Web of Conferences
dc.relationhttp://purl.org/au-research/grants/arc/FL110100098
dc.relationhttp://purl.org/au-research/grants/arc/FT120100760
dc.relationhttp://purl.org/au-research/grants/arc/DP130101569
dc.relationhttp://purl.org/au-research/grants/arc/DP140101337
dc.relationhttp://purl.org/au-research/grants/arc/DP160101254
dc.relationhttp://purl.org/au-research/grants/arc/DE140100784
dc.relation.ispartofseries2015 Heavy Ion Accelerator Symposium, HIAS 2015
dc.rights© The Authors, published by EDP Sciences. This is an open access article distributed under the terms of the Creative Commons Attribution License 4.0 (http://creativecommons.org/licenses/by/4.0/).
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.sourceEPJ Web of Conferences
dc.titleMass-asymmetric fission in the ⁴⁰Ca+¹⁴²Nd reaction
dc.typeConference paper
dcterms.accessRightsOpen Accessen_AU
local.contributor.affiliationEdayillam, Prasad, College of Science, ANUen_AU
local.contributor.affiliationHinde, David, College of Science, ANUen_AU
local.contributor.affiliationWilliams, Elizabeth, College of Science, ANUen_AU
local.contributor.affiliationDasgupta, Mahananda, College of Science, ANUen_AU
local.contributor.affiliationCarter, Ian, College of Science, ANUen_AU
local.contributor.affiliationCook, Kaitlin, Joint Colleges of Science, ANUen_AU
local.contributor.affiliationJeung, Dongyun, College of Science, ANUen_AU
local.contributor.affiliationLuong, Duc Huy, College of Science, ANUen_AU
local.contributor.affiliationMcNeil, Steven, College of Science, ANUen_AU
local.contributor.affiliationPalshetkar, Chandani, College of Science, ANUen_AU
local.contributor.affiliationRafferty, Dominic, College of Science, ANUen_AU
local.contributor.affiliationSimenel, Cedric, College of Science, ANUen_AU
local.contributor.affiliationWakhle, Aditya, College of Science, ANUen_AU
local.contributor.affiliationRamachandran, K., Bhabha Atomic Research Centreen_AU
local.contributor.affiliationKhuyagbaatar, J., Helmholz Institute Mainzen_AU
local.contributor.affiliationDullmann, Ch.E., Helmholz Institute Mainzen_AU
local.contributor.affiliationLommel, B., GSIen_AU
local.contributor.affiliationKindler, B., GSIen_AU
local.contributor.authoremailu5659091@anu.edu.auen_AU
local.contributor.authoruidEdayillam, Prasad, u5659091en_AU
local.contributor.authoruidHinde, David, u8203491en_AU
local.contributor.authoruidWilliams, Elizabeth, u5199930en_AU
local.contributor.authoruidDasgupta, Mahananda, u9206549en_AU
local.contributor.authoruidCarter, Ian, u5066232en_AU
local.contributor.authoruidCook, Kaitlin, u4661005en_AU
local.contributor.authoruidJeung, Dongyun, u4649176en_AU
local.contributor.authoruidLuong, Duc Huy, u4375034en_AU
local.contributor.authoruidMcNeil, Steven, u4534830en_AU
local.contributor.authoruidPalshetkar, Chandani, u5457231en_AU
local.contributor.authoruidRafferty, Dominic, u5235648en_AU
local.contributor.authoruidSimenel, Cedric, u4787848en_AU
local.contributor.authoruidWakhle, Aditya, u4182465en_AU
local.description.notesImported from ARIESen_AU
local.description.refereedYes
local.identifier.absfor020202 - Nuclear Physicsen_AU
local.identifier.ariespublicationa383154xPUB5952en_AU
local.identifier.doi10.1051/epjconf/201612303006en_AU
local.identifier.scopusID2-s2.0-85012918114
local.identifier.thomsonID000387536400020
local.identifier.uidSubmittedBya383154en_AU
local.type.statusPublished Versionen_AU

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